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1.
氧化锌纳米微晶的顺磁共振特性   总被引:16,自引:0,他引:16  
半导体纳米微粒是制备新一代电子器件的理想材料[1,2].电子自旋共振谱(ESR)是研究纳米微晶表面电子自旋构象和表面结构的一种有效方法.体相ZnO是一种抗磁性物质,通常观察不到顺磁共振信号(ESR).有关ZnO纳米微晶电子顺磁共振特性研究还未见文献报导.本文ZnO纳米微晶是用微乳法制备的:这样就制成了纳米尺度的具有表面包覆的ZnO微粒有机溶胶.这里表面活性剂起着“空间位阻”作用,一方面防止成胶过程中粒子间的聚合,使胶粒均匀细小;另一方面,包覆能减少微粒表面缺陷,使粒子性质变得十分稳定.将上述制得的ZnO纳米微粒…  相似文献   

2.
有机分子膜层间相互作用对聚集体的影响   总被引:1,自引:0,他引:1  
有机材料在分子设计与合成方面具有高度可塑性、灵活性及多样性,易于制成各种功能器件.带有电子给体和受体以及、电子体系的两亲类有机分子具有极高的超分子极化率“‘.利用Langmuir-Blodgett(LB)技术可实现有机材料在纳米尺寸上的分子组装,形成高度有序、非中心对称的LB膜以实现大的宏观二阶非线性极化系数.有机分子在LB膜中常常形成聚集体,而聚集体的存在将显著改变膜的宏观光学特性.根据有机分子间相互作用能的类型,聚集体可以分为J一型和H一型两种,分别表现为它们的吸收或荧光光谱‘”相对于单体发生红移或蓝移.近年来…  相似文献   

3.
聚合物Janus微粒是指具有各向异性微观结构的微/纳米聚合物粒子。因在乳液稳定、聚合物混合、可控组装、生物医药、多相催化和功能涂层等领域有重要的应用价值,聚合物Janus微粒材料的可控制备和应用研究已成为新型多功能和智能高分子材料研究的前沿领域。本文首先归纳了聚合物Janus微粒在制备方法、环境响应类型和应用领域的最新进展,进而分析了不同制备方法的优缺点。表面选择性修饰、微流体合成技术、自组装和种子聚合等方法都可用于制备具有可控尺寸、微观结构和表面性质的聚合物Janus微粒,但纳米级微粒微观结构的精确控制和大量合成还存在一定的挑战。环境响应性多组分聚合物Janus微粒在自组装和药物控释方面有其特殊的优势,而简单高效的种子聚合法有望应用于工业生产聚合物Janus固体表面活性剂。预计天然和多功能型聚合物Janus微粒的制备和应用研究将会是未来发展的趋势。  相似文献   

4.
近年来LB膜技术和超微粒子研究的发展,将两者有效地结合起来组装了与量子电子学、非线性光学、光电化学、化学生物传感器有关的纳米量级无机半导体材料[‘-‘j.其中TIO。纳米薄膜材料已在太阳能电池反射膜、压电铁电薄膜、电致显示器件[‘j、可逆光电池和超导薄膜[’]研究中都显示了广阔的应用前景.这类薄膜制备多采用化学气相沉积(CVD)技术和原子层外延.也有人把LB技术应用于纳米粒子的组装来制备TIO。超薄膜[”’j二本文利用烷氧基钛在水/空气界面上发生的溶胶一凝胶化反应制备TIO。基胶态粒子及其固态凝聚膜,将其与…  相似文献   

5.
Zn(Oxin)2·2H2O纳米晶的固相化学反应合成及表征   总被引:4,自引:0,他引:4  
随着纳米微粒研究的深入,对纳米超细微粒提出了不同的物理、化学特性需求,制备高纯、超细、均匀的纳米微粒,发展新型的纳米材料,就显得非常重要,而解决问题的关键在于研究、发展新的合成技术.通常,纳米微粒制备的要求是:表面洁净;粒子形状及粒径、粒度分布可控,防止粒子团聚;易于收集;有较好的稳定性;产率高.  相似文献   

6.
采用胶体化学法制备了稳定的SnO2纳米粒子(nanoparticleNP)水溶胶,用膜天平和原位布儒斯特角显微镜(BAM)考察了经典成膜材料花生酸(AA)在此水溶胶气-液界面的成膜性,并用LB膜技术在不同基底上制得了单层和多层AA-Sno2NP复合LB膜,通过TEM、小角X-ray、IR和UV-VIS光谱,进一步考察了该有序组装体的结构和周期性,以及组装作中Sno2纳米粒子的形貌、粒度分布和表面聚集状态.结果表明,用这种方法能够制得粒度分布均匀、农致密的Sno2纳米粒子复合LB膜,并且多层复合膜具有良好的周期性.  相似文献   

7.
分别以室温离子液体1-丁基-3-甲基-咪唑四氟硼酸盐和1-己基-3-甲基.咪唑四氟硼酸盐为介质,采用有机化合物热分解的方法制备了尺寸和结构均可控的金属Ni纳米微粒.采用X射线衍射仪、透射电子显微镜和傅立叶红外光谱仪对所制备的样品进行了结构表征.X射线衍射结果表明:以1-丁基-3-甲基-咪唑四氟硼酸盐为介质制备的Ni纳米微粒具有立方相结构,而以1-己基-3-甲基-咪唑四氟硼酸盐为介质制备的Ni纳米微粒具有六方相结构.透射电子显微镜结果表明:随着反应原料浓度的不同所制备的纳米微粒具有不同的粒径.傅立叶红外光谱表明:离子液体不但作为反应的介质而且作为修饰剂修饰在了Ni纳米微粒的表面,从而有效地阻止了Ni纳米微粒的团聚和氧化。  相似文献   

8.
有机光学非线性材料在光计算和光通讯领域中有着非常广泛的应用前景[1,2].非中心对称结构是二阶非线性光学器件的基本要求之一,对于有机两亲光学活性分子而言,使用能够在分子尺度上实现有序组装的Langmuir-Blodgett(LB)技术,可以制备具有稳定而非中心对称结构的多层膜.一般说来,Y型结构的多层膜比X型或Z型更稳定.然而,由单一材料组成的Y型LB多层膜只能形成中心对称结构,因而对宏观二阶非线性极化率X(2)没有贡献.为了解决稳定性与非中心对称性的矛盾,我们可以将光学非线性活性材料(如半花菁染料)与非活性隔层材料…  相似文献   

9.
采用热分解方法,以醋酸镍为前驱体,以表面活性剂十八胺为溶剂、还原剂和稳定剂,在镍纳米微粒初生成时进行原位表面修饰,制备出接近单分散的镍微球.采用扫描电子显微镜、透射电子显微镜、X射线衍射仪、红外光谱仪等分析了产物的尺寸、形貌、晶体结构及成分.结果表明,所制备的镍微球具有面心立方结构,由分散性良好、尺寸为300~400nm的纳米微粒组成;其在有机介质中具有良好的分散性,同时保持磁性纳米微粒的特性,可望用于电磁屏蔽材料和吸波材料.  相似文献   

10.
近年来,利用LB技术制备电活性的有机超薄膜受到广泛的关注.导电LB膜的膜材料主要是含有受体化合物7,7’,8,8’-四氰基二亚甲基苯醌(TCNQ)的电荷转移复合物[1~3]以及给体分子[4,5],特别是四硫代富瓦烯(TTF)衍生物[6~8].尽管LB膜多由带长链的两亲性分子组装而成,但是对非两亲性TTF衍生物LB膜的研究[9~11]结果表明,引入长链烷基并非制备TTF类电荷转移复合物LB膜的先决条件.该结果极大地拓展了LB膜材料的研究范围.本文报道非两亲性TTF衍生物与花生酸混合导电LB膜的制备、结构表征与导电性能研究.1实验部分利用亚磷…  相似文献   

11.
稀土Eu(Ⅲ)双酞菁衍生物LB膜的荧光性   总被引:3,自引:0,他引:3  
合成了八-4-(四氢糠氧基)酞菁铕(Ⅲ),通过元素分析、红外光谱、质谱和紫外-可见光谱加以确认。测定了配合物的II-A曲线,证明它有很好的成膜性,Z型沉积形成的LB膜材料有很强的荧光响应,随着LB膜厚度的增加,荧光性增强。掺杂邻菲咯啉形成的混合LB膜,其荧光性比纯膜强。但不是邻菲咯啉加入的量越多荧光性越强。配合物:邻菲咯啉=1:10时(摩尔比),有最好的荧光行为。用电子光谱对LB膜的结构进行了表征  相似文献   

12.
8-羟基喹啉两亲配合物的LB膜及其电致发光器件研究   总被引:6,自引:0,他引:6  
制备了两亲配体N-十六烷基-8-羟基-2-喹啉甲酰胺(HL)十个配合物的LB膜。采用π-A等温线和小角X射线衍射等方法研究了这些LB膜的性质和结构。两亲配合物的单分子占有面积为(1.25±0.06)nm^2和(0.75±0.06)nm^2,分别对应于两亲分子中两个喹啉环平躺和环与环之间以一定的角度倾斜于气/水界面。LB膜内分子排列是二维有序的超晶格结构,双层高度(5.0±0.1)nm;LB膜具有导电各向异性,其平面和垂直直流电导率分别为10^-^5S.m^-^1和10^-^9S.m^-^1;LB膜的高荧光性质使之可以用作为电致发光器件的发光材料。以LaL~2(H~2O)~4Cl的LB膜为发光层的单层电致发光器件的驱动电压为9V,发光亮度330cd/m^2,为黄绿色发光。  相似文献   

13.
聚苯胺基LB膜的制备及气敏特性的研究   总被引:7,自引:0,他引:7  
以聚苯胺 (PAN)为原料 ,利用LB(Langmuir Blodgett)超薄分子膜技术 ,制备了不同层数的纯聚苯胺LB膜及聚苯胺与乙酸 (AA)混合 (PAN AA)LB膜 ,对其进行了紫外 可见光光谱分析研究 ,并对不同层数的聚苯胺基LB膜的二氧化氮 (NO2 )气敏特性进行了研究 ,发现PANLB膜较PAN AALB膜具有更好的敏感性、响应性和可逆性 ,3层和 15层PANLB膜对相对百分比为 2 0× 10 -6NO2 的响应时间分别为 10s和 30s,15层PANLB膜的恢复时间约为 4min  相似文献   

14.
Cadmium sulphide (CdS) nanoparticles were grown by the reaction of sodium sulphide (Na2S) with Langmuir-Blodgett (LB) films of cadmium salts ofn-octadecylsuccinic acid (ODSU) and with LB films of ODSU in mixtures of octadecylamine and octadecyl alcohol. The results indicate that heterogeneous nucleation and aggregation in the pure ODSU LB films due to processes like Ostwald ripening are destabilized by the presence of the long-chain amine and alcohol in mixed systems. CdS nanoparticles in the LB films were monitored by UV-visible absorption spectra, which allow an estimation of the size of the particles. The morphology, size and nature of the nanocrystallites formed depend on whether the sulphidation was done on the pure film or in the mixed films. It is seen that particles of size around 1.6 nm were formed in ODSU/octadecylalcohol and ODSU/ octadecylamine mixed LB films while in pure ODSU films the size was about 2.7 nm. These films showed typical needle-shaped structures, as observed by the optical microscopic technique. Mean size and morphology were confirmed by transmission and scanning electron microscopy, while selective area electron diffraction patterns showed six-fold symmetry and indicated that the CdS crystals grow epitaxially with respect to the monolayer. Further, the crystallisation enhanced in the mixed LB films showed a characteristic zinc oxide (Wurtzite) structure compared with the pure ODSU matrix.  相似文献   

15.
稀土螯合物发光体LB膜的研究(I)   总被引:2,自引:0,他引:2  
稀土有机配合物的发光研究近年来取得了可喜的近展.铕(Ⅲ)、铽(Ⅲ)、钐(Ⅲ)与β-二酮(β-dik),三正辛基氧化膦(TOPO)所形成的螯合物,以及它们的硝酸盐与邻菲咯啉(Phen)所形成的螯合物都是高光效的发光体,有广阔的应用前景,在某些方面已获得应用.如能把这些具有发光功能的稀土螯合物组装成有序的分子组合体,则很可能在分子光学技术,光电子技术等领域发挥重要作用.如何组装?本文用LB 膜技术,通过交替成膜或混  相似文献   

16.
We examined the phase-separated structures of the mixed Langmuir-Blodgett (LB) films of C(k)H(2k+1)COOH (HkA: k=17, 21) and C(m)F(2m+1)C(10)H(20)COOH (FmH10A: m=6, 8) fabricated isothermally or after isobaric thermal treatments. Under isothermal fabrication conditions, disks and wire-type domains formed in the H17A/F6H10A LB films at high and low fabrication temperatures, respectively, because the line tension and dipole-dipole interaction were comparable with each other. The thermodynamically stable phases of H21A/F6H10A LB films at high and low fabrication temperatures were disks and polygonal domains, respectively. Isobaric thermal treatments of the Langmuir films affected the domain size and not the domain shape when the transfer temperature was the same. Isobaric thermal treatments were effective in controlling the domain size. The thermodynamically stable phases of both H17A/F8H10A LB films and H21A/F8H10A LB films were nanowires in the range of the fabrication temperatures studied. Isobaric thermal treatments of the Langmuir films did not affect the domain shape significantly and affected the domain size in both the LB films studied. The change in the value m of FmH10A was more effective in controlling the phase-separated structures of the mixed LB films than the value of k of HkA.  相似文献   

17.
Langmuir-Blodgett (LB) films at different mole fractions of p-terphenyl have been prepared using two different matrices, viz., stearic acid (SA) and polymethyl methacrylate (PMMA). Multilayered LB films have been formed by changing various LB parameters namely, mole fraction of mixing, changing the number of layers as well as also the different surface pressure of lifting. The spectroscopic characteristics of mixed LB films, solution and microcrystal have been compared using UV-vis absorption and steady state fluorescence spectroscopy. Change of planarity of TP molecules are occurred while going from solution to solid states/films. Fluorescence spectra of the mixed LB films reveal intense excimeric emission in the mixed LB films with D1 excimer peak at 397 nm and D2 excimer peak at 412 nm. Various LB parameters namely changing the number of layers as well as the different surface pressure of lifting played important roles in the formation of dual excimeric sites in the mixed LB films.  相似文献   

18.
The synthesis of a poly(azo)urethane by fixing CO(2) in bis-epoxide followed by a polymerization reaction with an azodiamine is presented. Since isocyanate is not used in the process, it is termed "clean method" and the polymers obtained are named "NIPUs" (non-isocyanate polyurethanes). Langmuir films were formed at the air-water interface and were characterized by surface pressure vs mean molecular area per mer unit (Pi-A) isotherms. The Langmuir monolayers were further studied by running stability tests and cycles of compression/expansion (possible hysteresis) and by varying the compression speed of the monolayer formation, the subphase temperature, and the solvents used to prepare the spreading polymer solutions. The Langmuir-Blodgett (LB) technique was used to fabricate ultrathin films of a particular polymer (PAzoU). It is possible to grow homogeneous LB films of up to 15 layers as monitored using UV-vis absorption spectroscopy. Higher number of layers can be deposited when PAzoU is mixed with stearic acid, producing mixed LB films. Fourier transform infrared (FTIR) absorption spectroscopy and Raman scattering showed that the materials do not interact chemically in the mixed LB films. The atomic force microscopy (AFM) and micro-Raman technique (optical microscopy coupled to Raman spectrograph) revealed that mixed LB films present a phase separation distinguishable at micrometer or nanometer scale. Finally, mixed and neat LB films were successfully characterized using impedance spectroscopy at different temperatures, a property that may lead to future application as temperature sensors. Principal component analysis (PCA) was used to correlate the data.  相似文献   

19.
用2-硝基-5-(N-甲基-N-十八烷基)氨基苯甲酸(NMOB)和花生酸制备了200层的交替多层膜, 测得其二次谐波信号强度与NMOB层数的平方成正比。论文着重讨论了NMOB的Y型膜和它与花生酸的交替膜中的取向, 并对两者之间的不同作了初步的解释。  相似文献   

20.
Structural and optical properties of multilayer Langmuir-Blodgett (LB) films of two amphiphilic carbenium salts 2-didecylamino-6,10-bis(dimethylamino)-4,8,12-trioxatriangulenium hexafluorophosphate (ATOTA-1) and 2,6-bis(decylmethylamino)-10-dimethylamino-4,8,12-trioxatriangulenium hexafluorophosphate (ATOTA-2) are described. The LB films were prepared on lipophilic glass by standard vertical dipping. Grazing incidence X-ray diffraction (GIXD) measurements show that the planar organic cores, in spite of their positive charge, form closely packed columns with a repeating distance of ~3.45 ?. Specular X-ray reflectivity (SXR) reveals the LB multilayers to consist of Y-type bilayers with thickness 31 ? for ATOTA-1 and 41 ? for ATOTA-2. This significant difference is ascribed to the different packing motifs of the alkyl chains in the two LB films. GIXD and polarized UV-vis absorption and emission spectroscopy show that the columnar aggregates in the LB films are oriented along the dipping direction. This alignment is attributed to shear effects during LB transfer. The main absorption band of the LB films is blue-shifted compared to that in solution, while the fluorescence is red-shifted by more than 100 nm. These findings suggest the presence of H-aggregates in agreement with the cofacial packing derived from the X-ray measurements. Polarized absorption spectroscopy with variable angle of incidence was used to resolve two perpendicular optical transitions in the visible range, one at 460 nm polarized perpendicular to the columnar direction, in the plane of the film, and one at 420 nm polarized along the film normal.  相似文献   

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